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Volumn 66, Issue 5, 2002, Pages 14-

Rotation due to hydrodynamic interactions between two spheres in contact

Author keywords

[No Author keywords available]

Indexed keywords

BUOYANCY; CONTACTS (FLUID MECHANICS); FRICTION; GRAVITATIONAL EFFECTS; INTERFEROMETRY; KINETIC ENERGY; REYNOLDS NUMBER; ROTATION;

EID: 41349087704     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.66.051504     Document Type: Article
Times cited : (10)

References (60)
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    • For example, the numerical algorithms from Refs. 21 22 may be generalized to evaluate the influence of the contact interactions on a modification of the three-particle contribution to the self-diffusion and to the suspension sedimentation velocity
    • For example, the numerical algorithms from Refs. 2122 may be generalized to evaluate the influence of the contact interactions on a modification of the three-particle contribution to the self-diffusion and to the suspension sedimentation velocity.
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    • When this manuscript was under review, we learned about another paper 57, in which the relative rotational motion of two sedimenting spheres had been analyzed theoretically and experimentally
    • When this manuscript was under review, we learned about another paper 57, in which the relative rotational motion of two sedimenting spheres had been analyzed theoretically and experimentally.
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    • Note that (Formula presented) is not equal to the mobility matrix (Formula presented) defined in Refs. 6 10
    • Note that (Formula presented) is not equal to the mobility matrix (Formula presented) defined in Refs. 610.
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    • The accuracy of the numerical derivative is higher than the difference between the experimental and theoretical points in Figs. 88 and 99. A change for (Formula presented) or (Formula presented) results in a shift of the points in Figs. 88 and 99, which is of the order of the maximal difference between the experiment and the model in Fig. 88, and in Fig. 99 for (Formula presented) The numerical derivatives with (Formula presented) and (Formula presented) are practically the same
    • The accuracy of the numerical derivative is higher than the difference between the experimental and theoretical points in Figs. 88 and 99. A change for (Formula presented) or (Formula presented) results in a shift of the points in Figs. 88 and 99, which is of the order of the maximal difference between the experiment and the model in Fig. 88, and in Fig. 99 for (Formula presented) The numerical derivatives with (Formula presented) and (Formula presented) are practically the same.
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    • T. Pastureaud and H. Kordoghli, report, 1998 (unpublished).


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